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>> During this third module, we are discussing techniques

for the acceleration and detection of elementary particles.

For this video, we are invited to hall SM18 of CERN, a hall where

the magnets of the Large Hadron Collider have been tested in the past and

spare magnets are still being checked out.

A part of this hall has been transformed into an exhibition.

At the end of this module, you will know how to describe the elements

of an accelerator and know how they look like in real life.

So, let us meet today’s host.

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For this video, we are accompanied by

Tobias Golling, who is one of my colleagues,

professor at University of Geneva, who dedicates 100% of his

research to the analysis of data from the ATLAS experiment at the LHC.

So, Tobis,

can you let us know what exactly you are doing in this domain?

>> Yes, with pleasure.

In short, I try to find new phenomena in the data,

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with my group.

Let me put this in context. The Standard Model is a great success,

it describes all visible matter, all forces, well almost all forces.

>> Except one.

>> Yes, except one.

The Higgs mechanism describes how all

particules acquire a mass, and the Higgs boson has been discovered

at CERN in 2012, so all of this is very, very well set.

But, there are weaknesses of the model.

For example, it cannot explain dark matter and it cannot explain

gravity, that his the missing force, and there are other phenomena, like, for example,

the famous hierarchy problem, i.e.

>> the difference in scale…

>> exactly, between the Higgs mass and the scale of gravity.

So, there are open questions. What are we to do?

We can ask our theorist colleagues,

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and they formulate hypotheses, that there are particles,

that one must introduce particles beyond the Standard Model,

and the hypothesis is that one can create these new

particle in our collisions. So I dedicate

my research to finding new particles,

like particles predicted by supersymmetry, or theories with extra dimensions.

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>> So, for this, the predicted cross sections

are very, very small, are they not?

>> They are of the order of, or smaller than the cross sections

characterising the Standard Model, and thus

we evidently need an high performance accelerator, a collider.

>> So, what are the properties of the LHC,

which are crucial for your research?

>> We expect that these particles have a very large mass,

and that their production rate is very low.

So, the two most important parameters of the LHC for this

are the energy and the luminosity.

Higher energy allows us to produce more massive particles.

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>> The LHC is a sort of double accelerator and

storage ring, where the protons circulate in two directions.

So, in principle, it is two accelerators in one, isn’t it?

>> Exactly. We have the principle of two-in-one, for all the magnets of the LHC

there are two coils.

>> Why does one need two accelerators?

>> Because there are two proton beams in opposite directions.

So, one needs two magnetic fields.

>> One beam circulates in one direction. >> Yes.

>> And the other in the opposite direction.

And they meet at the interaction points.

>> Yes.

We need the same Lorenz force towards the center of the orbit,

so we need one magnetic field pointing upwards, the other one downwards.

And for this one uses these dipole magnets.

>> So here, we are almost sitting on one of these dipole magnets,

Can you explain the elements of these magnets a little?

>> Exactly.

So here, one sees the two rings, the two vacuum tubes,

and one sees two coils, one and the other, which are exactly the same,

the only difference is that the current is reversed.

And here is the common yoke for the magnetic fields

and the cryostat is also in common.

>> Ok.

So, in one of these coils, there is an upward pointing magnetic field,

and in the other, the same dipole field, but pointing downward.

With means that we are deviating the two beam in the same direction,

even though they have opposite directions, simply

applying Lorentz’ law, which gives the centripetal force,

which we need, q(v x B) in this case.

>> Exactly,

with the right hand rule.

>> Mh mh.

The two coils are in the same cryostat. Why?

Why does one not simply build two separate magnets?

>> One can reduce the cost this way,

having a common cryostat for the two coils.

>> So, for the enormous energies of the

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>> Exactly.

>> Ok.

And because of that, all are in one cryostat.

So, the coils themselves are made of copper, aren’t they?

>> Maybe a few numbers about the magnetic system,

which show that it is really very important,

even essential for the LHC.

Of the 27 km of circumference, 85% are

occupied by magnets, the magnet system… >> Ok.

>> …and 75% by dipoles, like this one.

>> So this is really the heart of the matter.

Magnets are practically everywhere.

>> There are magnets everywhere, right.

There are more than 1000, more than 1200 elements like this.

Each one weighs 30 tons,

has 15m length and a maximum magnetic field of 8.3 Tesla.

>> So what we see here is just a small segment of a dipole,

which in reality is much longer.

>> Ok.

So this makes a gigantic cryogenic system,

so, practically all the ring is at cryogenic temperature,

all around its length of 27km.

>> Yes.

So, later we will see the superconducting cables, there are 1200 tons of

superconducting cables and it needs 130 tons of superfluid helium

to cool down all this mass to 1.9 Kelvin.

>> Wow.

>> So I propose to move on to see

how these coils look and

also the focalising elements of the LHC.

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of the accelerator, Tobias?

>> So, here we come back to the luminosity, which we have already mentioned.

The luminosity is inversely proportional

to the common surface of the two proton beams,

and that is why one must focalise them, to reduce this surface.

And here we see very well

a section of a quadrupole magnet, which is responsible for the focalisation.

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One sees very well the four poles, here two north poles and two south poles, and then

here are two version of this magnet, one is responsible for

horizontal focalisation, the other one for the vertical one.

One alternates the two…

>> Puts them in chains.

>> …to have an optimum focalisation.

>> So if we look at the coils, the wires go effectively

in this direction, don’t they?

>> Exactly. >> So here we have in fact

a section of such a coil. Can you

explain the ingredients of such a coil?

>> Yes.

All coils are composed of superconducting cables, they are very important,

as we said, there are 1200 tons of these cables.

They are in fact composed of these strands, with a diameter of roughly 1mm.

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>> And all of this is normally imbedded in a sort of aluminum stabiliser,

that is why there is this gray material.

>> Yes, yes.

>> OK. So this serves to wind the coils of the active part

of the magnets.

But also to transport current around the accelerator, doesn’t it?

>> Exactly.

We have these cables all around the accelerator.

If one takes the total length of the filaments,

one arrives at an astronomical scale.

One can go five times to the sun an back with this.

>> It is really incredible, all this effort

which is made to produce the particles

you are searching for, isn’t it?

>> In fact it serves this purpose.

>> So, we still need to discuss an element of the accelerator

which we have not covered yet.

These are the accelerating elements themselves.

So I propose that we move on to see what they look like in reality.

In this small video animation we see a cryostat which contains four

superconducting elements, i.e. radio frequency resonators.

The radio frequency wave enters through these wave guides

and establishes an electric field with the right polarity, such that

the beam is accelerated in its direction of motion.

So here is one of these elements.

Tobias, can you please explain these ingredients of this

radio frequency cavity?

>> Of course. Such a cavity has

as you said, the principle purpose to accelerate protons

from an energy of 450 GeV,

the energy with which they enter the LHC,

up to 7 TeV, which is their maximum energy.

Here we see the wave guides, the radio frequency

generated by the Klystron enter here and leaves there.

For the LHC, they have a frequency of 400 MHz.

>> OK.

So inside, a stationary wave is formed.

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And when the polarity is right at the right time of arrival of the protons,

we will have a net acceleration in the direction of the electric field.

So, how does one synchronise this wave with the beam passage?

>> It is very important to have mono-energetic beams

So we must equalise the proton energy.

So when the proton with the right energy

enters at the right moment, there will be no acceleration

if we are already at the maximum energy level.

However, if the protons arrive too early or too late,

i.e. when their energy is a little too large or too small, an acceleration is felt

the protons are decelerated or accelerated to approach the ideal energy.

This happens automatically, when the protons enter in the increasing

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phase of the electric field, as we have seen in video 3.2.

So, this accelerating cavity, the resonator and all what is around,

is made of copper and is emerged in a cryostat, which holds

it at liquid helium temperature, such that the copper is superconducting.

>> So why is it important that this structure

also is superconducting?

>> Yes, it is very important that there is a minimum

ohmic resistance, such that the power

of the wave is not attenuated.

>> Ok, this means that the radio frequency wave

arrives without loss from the klystron to the beam.

>> Exactly.

>> Ok.

So, thank you very much, Tobias, for this visit,

and for this demonstration of the LHC elements.

This concludes this video.

In the next video,

we will start to discuss particle detection.

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